electromagnetic simulations of vmtsa equipped with the rf fingers and ferrites
DESCRIPTION
Electromagnetic Simulations of VMTSA Equipped with the RF Fingers and Ferrites. O. Kononenko CERN, BE/RF JINR Thanks to Benoit Salvant, Alexej Grudiev, Elias Métral LRFF Meeting, CERN, October 30, 2012. Outline. - PowerPoint PPT PresentationTRANSCRIPT
Electromagnetic Simulations of VMTSA Equipped with the
RF Fingers and Ferrites
O. KononenkoCERN, BE/RF
JINR
Thanks to Benoit Salvant, Alexej Grudiev, Elias Métral
LRFF Meeting, CERN, October 30, 2012
2
Outline
• Realistic finger deformations for VMTSA equipped with the longer fingers. Time domain, eigen frequency and wire simulations
• Simulations of the deformed shorter fingers and effect of Philips 8C11 ferrites
3
RF Fingers Deformation in VMTSA
4
Simulated VMTSA models
Conforming fingers
Wire,conforming fingers
Wire,no fingers Bad contact
2st type
Deformation+Ferrites
Wire,20-50mm gaps
Completed In progress
Old longer fingers New shorter fingersConforming and bad contactfingers
Bad contact 1st type
5
VMTSA with Wire and Comforming Fingers
Port 1
Port 2
Copper
Perfect H Model:
- 180 deg of the structure- copper outer walls
Simulation profile: - second order basis functions
- curvilinear elements enabled- discrete sweep from 20MHz to 2GHz, 20MHz step- 0.01 s-parameters accuracy => ~220K tet10 mesh
Wire
- no matching
6
VMTSA with Wire and Deformed Fingers: 20-40mm gaps
Port 1
Port 2
Copper
Perfect H Model:
- 180 deg of the structure- copper outer walls
Simulation profile: - second order basis functions
- curvilinear elements enabled- discrete sweep from 20MHz to 2GHz, 20MHz step- 0.01 s-parameters accuracy => ~260K tet10 mesh
Wire
Gap: 20-40mm
Gap- no matching
7
VMTSA with Wire andMore Realistic Deformation
Port 1
Port 2
Stainless Steel
Perfect H Model:- 180 deg of the structure- copper outer walls
Simulation profile: - second order basis functions
- curvilinear elements enabled- discrete sweep from 10MHz to 2GHz, 10MHz step- 0.01 s-parameters accuracy => ~300K tet10 mesh
Wire
Gap: 40-50mm
Gap- no matching load
8
Transmition for Different Gap Sizes
0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2-35
-30
-25
-20
-15
-10
-5
0
Frequency, GHz
S 21, d
B
40 mm50 mm
Different level of transmission probably because there is no matching load in the HFSS simulation
9
CST TD Simulations of VMTSA Model:
- full structure- copper walls- conforming fingers and 40-50 mm gap
Simulation profile: - 10 lines per wavelength - refine at PEC by factor 6 - 70mm bunch sigma
- 400K hex mesh
10
Longitudinal Impedance
11
Longitudinal Wake Potential
12
Ht for Bunch Passage through VMTSA
13
Power Spectrum Measurements
HFSS Eigen Mode Analysis: 40mm
14
Mode Complex Magnitude
Eigen Frequency
[MHz]Q-factor
Shunt Impedance,
[Ω]Power Loss
[W]
1 279 455 10050.5 652.8
2 342 211 192.6 12.5
3 370 163 7.5 0.6
4 383 134 1.7 0.1
5 390 114 0.6 0.04
WV
QR zL
2
dVEEWV
*0
2
dzefzEVL
czizz
0
/),(
Longitudinal Shunt Impedance
Voltage along the beam path
Energy stored in the volume
15
HFSS Eigen Mode Analysis: 50mm
Mode Complex Magnitude
Eigen Frequency
[MHz]Q-factor
Shunt Impedance
[Ω]Power Loss
[W]
1 270 387 7121.6 462.6
2 330 145 50.2 3.3
3 362 147 7.2 0.6
4 380 127 8.4 0.7
5 392 115 3.1 0.2
16
Surface Loss Density for the First Eigen Mode @ 279 MHz
Log scale, 40 mm gap, eigen mode @ 279MHz with 10KΩ longitudinal shunt impedance
17
Shorter RF FingersHFSS Simulation Setup: Eigensolver
Perfect H
Copper
Simulation profile: - second order basis functions
- curvilinear elements enabled- 1% frequency accuracy leads to ~300K tet10 mesh
Model:- 180 deg of the structure- copper outer walls- 10mm gap
10 mm gap
18
0.113 V/m
0.037 V/m
0.030 V/m
0.005 V/m
0.028 V/m
Shorter RF Fingers, CmplxMag(E)
Mode 1
Mode 2
Mode 3
Mode 4
Mode 5
Eigenmodes of the Bellows
19
Eigen Frequency, MHz
Q-factor Shunt Impedance, Ω
Power Loss,W
HFSS CST HFSS CST HFSS CST HFSS CST
Mode 1 339 339 2409 32 50709 676 2616 87
Mode 2 526 531 1872 322 8442 1438 275 186
Mode 3 549 550 6023 6837 0 0.03 0 0.004
Mode 4 586 583 2462 155 196 7 5 0.907
Mode 5 670 - 1217 - 389 - 5 -
Eigen Modes, Shorter RF Fingers
20
VMTSA equipped with Ferrites
4 pieces of Philips 8C11 (60x30x5 mm) were installed in one VMTSA module equipped with the shorter fingers
21
Philips 8C11 Ferrite: Permeability
10-3 10-2 10-1 100100
101
102
103
Frequency, GHz
Perm
eabi
lity
http://www.ferroxcube.com/appl/info/HB2009.pdf
22
Philips 8C11 Ferrite: Resistivity and Permittivity
10-3 10-2 10-1 100 101 10210
20
30
40
50
60
70
80
90
100
Frequency, MHzR
elat
ive
Perm
ittiv
ity
10-1 100 101 1020
1
2
3
4
5
6
7
8
9
10x 104
Frequency, MHz
Res
istiv
ity,
m
http://www.ferroxcube.com/appl/info/HB2009.pdf
23
HFSS Setup
Perfect H
Copper
Simulation profile: - second order basis functions
- curvilinear elements enabled- 1% frequency accuracy
Model:- 180 deg of the structure- copper outer walls- 10mm gap- 4 ferrite pieces
10 mm gap
Ferrite 8C11
24
New Fingers Ferrites 10mm Mode Eigen Frequency
[MHz]Q-factor Shunt
Impedance [Ω]
Power Loss[W]
1 133 1 0.239 0.019544
2 133 1 0.007 0.000572
... ... ... ... ...
3 341 2479 52455 2706
... ... ... ... ...
4 528 1867 8401 316
... ... ... ... ...
Many modes excited in the vicinity of ferrites and in the area outside the conforming fingers. Some modes excited near to the gap and not affected by ferrites at all
25
Eigenmodes, CmplxMag(E)
133 MHz
133 MHz
341 MHz
528 MHz
Mode 1
Mode 2
Mode 3
Mode 4
26
Surface Loss Density for the First Eigen Mode @ 341 MHz
Linear scale, 10 mm gap, eigen mode @ 341MHz with 2700 W power losses
27
Conclusions
• Different shapes of the finger deformations have been studied for longer and shorter fingers. Unconformities could result in ~kW power losses => enough to melt fingers.
• Ferrites in the proposed position and amount don’t help. Additional dedicated study is necessary to see if we can damp modes with ferrites.